光学学报, 2018, 38 (8): 0830001, 网络出版: 2018-09-06
半球形空腔约束等离子体的时空演变特性研究 
下载： 902次
Temporal and Spatial Evolution Characteristics of Plasma Confined by Hemispherical Cavity
图 & 表
图 2. 无约束和半球形空腔约束下Fe I: 374.57 nm谱线强度的时间演变。(a) D=5 mm; (b) D=7 mm; (c) D=9 mm; (d) D=10 mm; (e) D=11 mm; (f) D=13 mm; (g) D=15 mm; (h) D=17 mm; (i) D=19 mm
Fig. 2. Temporal evolution of spectral line intensity of Fe I: 374.57 nm with and without hemispherical cavity confinement. (a) D=5 mm; (b) D=7 mm; (c) D=9 mm; (d) D=10 mm; (e) D=11 mm; (f) D=13 mm; (g) D=15 mm; (h) D=17 mm; (i) D=19 mm
图 3. 半球形空腔直径与最佳增强倍数对应采集延时的关系
Fig. 3. Relationship between the diameter of the hemispherical cavity and the delay time corresponding to the best enhancement factor
图 4. 半球形空腔直径与最佳增强倍数的关系
Fig. 4. Relationship between the diameter of hemispherical cavity and the best amplification of enhancement
图 5. 谱线强度的二维空间分布。(a)无约束, Fe I: 374.57 nm; (b)无约束,Fe II: 275.59 nm; (c)半球形空腔约束,Fe I: 374.57 nm; (d)半球形空腔约束, Fe II: 275.59 nm
Fig. 5. Two-dimensional spatial distributions of spectral line intensity. (a) Unconfined, Fe I: 374.57 nm; (b) unconfined, Fe II: 275.59 nm; (c) hemispherical cavity confinement, Fe I: 374.57 nm; (d) hemispherical cavity confinement, Fe II: 275.59 nm
李小龙, 王静鸽, 张利平, 李新忠. 半球形空腔约束等离子体的时空演变特性研究[J]. 光学学报, 2018, 38(8): 0830001. Xiaolong Li, Jingge Wang, Liping Zhang, Xinzhong Li. Temporal and Spatial Evolution Characteristics of Plasma Confined by Hemispherical Cavity[J]. Acta Optica Sinica, 2018, 38(8): 0830001.
PDF全文
